(a) i. The ground state was given in the problem.
ii. The first excited state corresponds to the absorption of the 400 nm photon. This energy is given by E = hc / λ … 1240/400 = 3.1 eV. Moving from a state of –5 eV and absorbing 3.1 eV moves you up to the higher excited state of –1.9 eV.
iii. After reaching the excited state, the electron makes two visible drops. It drops back down the ground state emitting the 400 nm photon, or it emits the 600 nm photon. This photon corresponds to an energy of 2.1 eV (found with E = hc / λ again). Starting at –1.9eV and emitting 2.1 eV would put you in the –4eV level.

(b) From the diagram above, the emission not yet analyzed is from the ‘other’ state to the ground state. That emission corresponds to an energy release of 1 eV. The λ of this emission can be found with E = hc / λ. Giving λ = 1240 nm. Since this is outside of the visible spectrum, it is not ‘seen’, but it does occur.